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Related Concept Videos

Double Resonance Techniques: Overview01:12

Double Resonance Techniques: Overview

Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis. This...
Atomic Nuclei: Magnetic Resonance01:05

Atomic Nuclei: Magnetic Resonance

The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
¹H NMR Signal Multiplicity: Splitting Patterns01:13

¹H NMR Signal Multiplicity: Splitting Patterns

When protons A and X are coupled, their nuclear spin energy levels are slightly modified. This is because the energy required to excite proton A to a spin state parallel to proton X is slightly different from the energy required for it to become anti-parallel to spin X. Consequently, there are two possible excitation frequencies for A (A1 and A2), depending on the spin state of X, and vice versa. The mutual nature of coupling implies that the difference between frequencies A1 and A2, indicated...
Standing Waves in a Cavity01:28

Standing Waves in a Cavity

A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
Magnetic Damping01:17

Magnetic Damping

Eddy currents can produce significant drag on motion, called magnetic damping. For instance, when a metallic pendulum bob swings between the poles of a strong magnet, significant drag acts on the bob as it enters and leaves the field, quickly damping the motion.
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External Excitation of Neurons Using Electric and Magnetic Fields in One- and Two-dimensional Cultures
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Magnetic and electric excitations in split ring resonators.

Jiangfeng Zhou1, Thomas Koschny, Costas M Soukoulis

  • 1Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA. jfengz@iastate.edu

Optics Express
|June 25, 2009
PubMed
Summary
This summary is machine-generated.

This study explores U-shaped split-ring resonators (SRRs), revealing higher-order electric and magnetic resonance modes. Magnetic resonances correspond to odd half-wavelengths, while electric resonances align with integer wavelengths.

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Area of Science:

  • Electromagnetism
  • Metamaterials
  • Nanophotonics

Background:

  • Split-ring resonators (SRRs) are fundamental metamaterial structures.
  • Understanding their electromagnetic resonance modes is crucial for device applications.

Purpose of the Study:

  • To investigate the electric and magnetic resonance modes in U-shaped SRRs.
  • To characterize higher-order excitation modes and their current distributions.
  • To analyze the dependence of electric and magnetic moments on SRR geometry.

Main Methods:

  • Theoretical analysis of U-shaped SRR electromagnetic resonances.
  • Identification of current distribution patterns for different resonance modes.
  • Mathematical formulation of electric and magnetic moments.

Main Results:

  • Higher-order electric and magnetic resonance modes were identified in U-shaped SRRs.
  • Magnetic resonances correspond to odd multiples of half-wavelengths (λ/2, 3λ/2, 5λ/2).
  • Electric resonances correspond to integer multiples of full wavelengths (λ, 2λ, 3λ).
  • The magnetic moment of magnetic resonance diminishes to zero as the SRR side arm length approaches zero.

Conclusions:

  • U-shaped SRRs exhibit complex resonance behaviors beyond fundamental modes.
  • The geometrical parameters, specifically side arm length, critically influence the magnetic resonance properties.
  • Simple rod structures lack magnetic resonance, highlighting the importance of the split-ring geometry.